rankine's thermodynamics. 483 if Sj be zero, we have H^Oj and work will bo done by an aclia- b^tic expansion, and in Fig. 24 we have: — S.i = 7nbbxml, … Then T, = ra and equation (E4) becomes kr^mavJL, = / *pdv— S2 + Sx. S,=MAaw, II / pdv In this case the last terms of equations (mz) and (nz) are equal, and. we have S=MBbm, -S3 + S1 = -NB51n, + MAalwl. • hence, (Equation E4), Professor Tait, an ardent admirer of our author says of him : " He was…
Engineering
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